| METALLURGICAL AND MATERIALS TRANSACTIONS B | |
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Volume 28B, No. 2, April 1997 This Month Featuring: Hydrometallurgy, Pyrometallurgy, Transport Phenomena, Process Control, Physical Chemistry, Solidification, Solid State Reactions, and Mathematical Modeling. View April 1997 Table of Contents.
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Communication: Discussion of "The Adsorption kinetics of Dycyanoaurate and Dycyanoargentate ions in activated Carbon"
N.M. VEGTER and R.F. SANDENBERGH
Rate Control of the Flash Reduction of Zinc Calcines
E.M. WEENINK and N.J. THEMELIS
This work was part of a feasibility study on the production of zinc by flash-reducing zinc calcines (approximately consisting of 60 pct Zn and 10 pct Fe). The rate of reduction of single pellets was determined and incorporated in a unidimensional mathematical model of the transport and chemical reaction phenomena in a flash reaction shaft. The final experimental stage was to flash-reduce zinc calcines in a 0.13-m i.d. x 1.2-m-high reaction shaft at feed rates of 1.5 to 3 kg/h and in a range of CO/CO2 mixtures, which represented the products of the carbon-oxygen reactions in an industrial reactor. It was found that the principal variable affecting the rate of reduction was the CO/CO2 ratio. The observed low rates of reduction of zinc calcine particles were in fair agreement with the projections of the mathematical model and were also confirmed by tests on a mini-pilot flash reactor (40 kg calcine/h), carried out by Outokumpu Research (Pori, Finland). The main conclusion was that the reduction process is chemically controlled at rates which are an order of magnitude less than the flash oxidation of sulfide concentrates. Therefore, the reaction shaft of a zinc flash reduction furnace must be considerably longer than for the conventional flash smelting of sulfide concentrates.
Critical Evaluation and Optimization of the Thermodynamic Properties and Phase Diagrams of the CrO-Cr2O3-SiO2-CaO System
SERGEI DEGTEROV and ARTHUR D. PELTON
Available thermodynamic and phase diagram data have been critically assessed for all phases in the CrO-Cr2O3-SiO2-CaO system from 298 K to above the liquidus temperatures at all compositions under reducing conditions and at low CaO concentrations under oxidizing conditions. All reliable data have been simultaneously optimized to obtain one set of model equations for the Gibbs energy of the liquid slag and all solid phases as functions of composition and temperature. The modified quasichemical model was used for the slag. The models permit phase equilibria to be calculated for regions of composition, temperature, and oxygen potential where data are not available.
Thermodynamics of Iron Oxide in FexO-Dilute CaO + Al2O3 + FexO Fluxes at 1873 K
HIROYASU FUJIWARA, MASAHIRO KITOU, TAKAYUKI MATSUI, and EIJI ICHISE
The distribution of iron between FexO-dilute CaO + Al2O3 + FexO fluxes and Pt + Fe alloys, as well as the redox equilibrium of iron ions in these fluxes, was experimentally investigated in pressure- controlled CO2/CO gas at 1873 K. Total iron content in flux (pct FeT) and the ratio of (pct Fe2+) to (pct FeT) in fluxes with constant XCaO/XAl2O3 can be related to the activity of iron, aFe, and the partial pressure of oxygen, pO2, using the following equation:


°FexO, relative to the liquid iron oxide in equilibrium with iron. Furthermore, the composition dependence of
°FexO is discussed.
Galvanic Cell Measurements on Supersaturated Activities of Oxygen in Fe-Al-M (M = C, Te, Mn, Cr, Si, Ti, Zr, and Ce) Melts
GUANGQIANG LI and HIDEAKI SUITO
Using a mullite (3Al2O3 · 2SiO2)-tube and ZrO2-9 mol pct MgO-plug type solid electrolyte galvanic cells, the activities of supersaturated oxygen in Fe-0.0017 to 0.41 mass pct Al-M (M = C, Te, Mn, Cr, Si, Ti, Zr, and Ce) alloys were measured as a function of total Al or M contents at 1873 K in an alumina crucible. Based on these results, the effects of alloying elements on the supersaturated oxygen activity with respect to alumina precipitation were studied. In the Fe-Al-M (M = C, Te, Mn, Cr, and Si) alloys, the supersaturated oxygen activities for a given Al level approach the equilibrium values with increasing contents of alloying elements. However, the oxygen activities for a given Al level are still supersaturated in the Fe-Al-M (M = Ti, Zr, and Ce) alloys even in the presence of considerable amounts of the alloying elements.
Effect of Alloying Element M (M = C, Te, Mn, Cr, Si, Ti, Zr, and Ce) on Supersaturation during Aluminum Deoxidation of Fe-Al-M Melts
Reduction of Molybdenite with Carbon in the Presence of Lime
Dissolution of Alumina in Mold Fluxes
GUANGQIANG LI and HIDEAKI SUITO
The effect of the alloying element M (M = C, Te, Mn, Cr, Si, Ti, Zr, And Ce) on the supersaturation of alumina precipitation in the Fe-0.0017 to 0.41 mass pct Al-M alloys was studied at 1873 K in an Al2O3 crucible based on the contents of analyzed aluminum and oxygen. It was found that the supersaturation ratio with respect ot the Al2O3 precipitation, S°Al2O3{=(aAl2 · aO3)obs/(aAl2 · aO3)eq}, decreased with increasing content of the alloying element in the Fe-Al-M (M = C, Te, Mn, Cr, and Si) alloys and approached unity in the range of [mass pct M]
0.2 to 0.5. In the Fe-0.011 to 0.41 mass pct Al-M (M = Ti, Zr, and Ce) alloys, however, the S°Al2O3 values were found to be independent of the contents of the alloying elements up to the compositions of [mass pct Ti] = 1.03, [mass pct Zr] = 0.08, and [mass pct Ce] = 0.07.
R. PADILLA, M.C. RUIZ, and H.Y. SOHN
The thermodynamics of the MoS2-C-CaO system has been studied in order to understand the carbothermic reduction of molybdenite in the presence of CaO. Kinetic studies were also conducted with mixtures of MoS2 + C + CaO in the temperature range of 900°C 1200°C. The reduction of MoS2 with carbon in the presence of lime proceeds through the direct oxidation of MoS2 by CaO to form intermediate molybdenum oxidized species, MoO2 and CaMoO4, which subsequently undergo reduction by CO to yield mixtures of Mo, Mo2C, and CaS. Complete conversion of MoS2 can be obtained at 1200°C in less than 20 minutes for molar concentrations of MoS2:C:CaO = 1:2:2. The kinetic model ln (1 - X) = kt was used to determine the rate constants. The activation energy found for the temperature range studied was 218.8 kJ/mol.
X. YU, R.J. POMFRET, and K.S. COLEY
The solubility and rate of dissolution of alumina in a range of mold fluxes in the CaO-Al2O3-SiO2-Na2O-CaF2 system have been measured at 1530°C using the rotating finger method. The solubilities were approximately 38 pct for all fluxes studied. The kinetics of dissolution were correlated with the Levich-Chochran equation for a rotating disc and used to determine the effective diffusivity of alumina. The effective diffusivity was inversely proportional to the viscosity of the flux and showed excellent agreement with previous work on CaO-Al2O3-SiO2 slags. This is in keeping with either the Eyring relation or the Stokes-Einstein relation. The value obtained for the size of the diffusing unit when the Stokes-Einstein relation was used, 1.81 Å, was more reasonable, which is not normally expected for silicate slags. This result is explained by the low level of polymerization in these fluxes.
SOLIDIFICATION
Calculation of Solidification-Related Thermophysical Properties for Steels
JYRKI MIETTINEN
Special algorithms have been developed to calculate important solidification-related thermophysical properties: enthalpy and enthalpy-related data (i.e., specific and latent heat), density, and thermal conductivity for low-alloyed and stainless steels. The algorithms are heavily based on the use of earlier developed phase transformation models, an interdendritic solidification model (IDS), and an austenite decomposition model (ADC), which solve, as a function of temperature, the phase fractions and compositions needed in these calculations. As a result, the thermophysical properties can be calculated at any temperature, from 1600°C to 25°C, taking into account the discontinuities caused by special phase transformations (i.e., ferritic, austenitic and peritectic solidification, ferrite/austenite transformation, and austenite decomposition to various structures) influenced by the steel grade and the cooling conditions.
Kinetics of Reduction of MnO in Powder Mixtures with Carbon
W.J. RANKIN and J.R. WYNNYCKYJ
Experimental data on the kinetics of the reaction between MnO and graphite in a mixture of fine powders, obtained earlier by one of the authors, were reassessed. The principal motive was to test on this system a new kinetic model, the "intrinsic transport" model, published previously by the present authors. In this model, the reaction-rate-limiting step is assumed to be transport of a gaseous intermediate by pore diffusion between reaction sites on the surfaces of the reactant particles. Various other model formalisms potentially applicable to this reaction also were tested. It is shown that the intrinsic transport of CO2 gave good to excellent fits to the experimental data over a wide range of reaction conditions. Other models gave poor agreement. It is shown, furthermore, that for the case where the CO2 pore-diffusion path lengths were made small (fine MnO and coarse graphite particle size), thus speeding up rapid intrinsic transport, the graphite-surface reaction became rate controlling.
Turbulence Model Predictions of Flowin a Continuous Casting Billet-Mold Water Model Using Laser Doppler Velocimetry Measurements
turbulence models. The predictive capabilities of these turbulence models were assessed in comparison to the experimentally measured axial velocity and turbulence kinetic energy values. The measured turbulence velocity fluctuations in various directions strongly suggest the non isotropic nature of the flow field, which cannot be predicted with the k-
models. The extent of deviations between the measurements and computations was quantified.
Modeling the Discontinuous Liquid Flow in a Blast Furnace
G.X. WANG, S.J. CHEW, A.B. YU, and P. ZULLI
This article presents a mathematical model to describe the discontinuous flow of an isothermal liquid in packed beds, simulating in part the flow condition in and below the blast furnace cohesive zone. The model is developed based on a force balance approach to describe the discrete liquid flow and a stochastic treatment to take into account the complex packing structure. The interaction between gas and liquid flows has also been included in the governing equations, so that the localized liquid flow in a packed bed can be modeled with or without gas flow. The difference between the micro scopic and macroscopic approaches is discussed, and it is argued that at this stage of development, liquid flow modeling should be conducted at the macroscopic level. Techniques for numerical so lution are provided. The validity of the proposed model is demonstrated by comparing model pre dictions with measurements obtained using a two-dimensional cold model apparatus under different gas and/or liquid flow conditions.
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